Beam steering with a periodic resonance structure

ABSTRACT

Method and apparatus for steering an antenna beam using a periodic resonance structure ( 300 ). The method can include the step of electrically and magnetically coupling a first fluid dielectric ( 114 ) to a plurality of transmission line stubs ( 104 ) that are respectively coupled to a plurality of radiating elemments ( 102 ) of a periodic resonance structure ( 300 ). The first fluid dielectric ( 114 ) is controlled to selectively vary an electrical length of each of the transmission line stubs ( 104 ). This permits directing an angle of a redirected RF beam produced by an incident RF signal ( 306 ) impinging on the periodic resonance structure ( 300 ).

BACKGROUND OF THE INVENTION

1. Statement of the Technical Field

The inventive arrangements relate generally to methods and apparatus forsteerable beam antennas, and more particularly to periodic resonancestructures that can be used for steering antenna beams.

2. Description of the Related Art

Periodic resonance structures may be found in a wide variety of RFapplications. One example of a periodic resonance structure is afrequency selective surface (FSS). An FSS is conventionally designed toeither block or pass electromagnetic waves at a selected frequency.These types of surfaces are essentially periodic resonance structuresthat are comprised of a conducting sheet periodically perforated withclosely spaced apertures, or may be comprised of an array of periodicmetallic patches. FSS structures can generally be separated into twobroad categories, namely inductive and capacitive type geometries. Aninductive FSS operates in a manner similar to a band-pass filter. Acapacitive FSS, behaves in a manner that is similar to a band-stopfilter. When the periodic elements comprising an inductive FSS are atresonance, the FSS will pass RF signals that are at or near the resonantfrequency. In contrast, the capacitive FSS will reflect signals at ornear the resonant frequency of the elements.

A typical capacitive FSS is constructed out of periodic rectangularmetal patches disposed on a planar substrate. By comparison, aninductive type FSS is typically constructed using periodic rectangularapertures which are formed by perforating a metal sheet that has beendeposited on a substrate. Many other types of FSS element configurationsare known, including circles, Jerusalem crosses, concentric rings,mesh-patch arrays or double squares supported by a dielectric substrate.Depending upon the geometry selected, these can combine features ofinductive and capacitive elements and can be used to provide desirablefrequency responses. U.S. Pat. No. 3,231,892 describes some basic FSSgeometries and one potential application for an FSS type periodicresonance structure. Notably, signals that are blocked by a FSS aretypically reflected away from the FSS, but the reflected direction isoften not a matter of concern for the designer.

Another type of periodic resonance structure is a reflectarray. Areflectarray is typically comprised of an array ofresonantly-dimensioned microstrip antenna radiator patches that areclosely spaced above a ground plane. Conventional electronic phaseshifters can be provided for shifting the phase of an incident RF signalreceived by each antenna radiator patch and then retransmitting thesignal, usually via the same antenna radiator patch. For example, diodeswitches can be used to control a transmission line structure to vary aphase shift. The phase shifts of the individual resonators create aphased array effect that can be controlled to determine the direction ofa redirected beam of RF energy. One example of a reflectarray isdisclosed in U.S. Pat. No. 4,684,952 to Munson et al. However,alternative arrangements are also known in the art.

SUMMARY OF THE INVENTION

The invention concerns a method for steering an antenna beam using aperiodic resonance structure. The method can include the step ofelectrically and magnetically coupling a first fluid dielectric to aplurality of transmission line stubs that are respectively coupled to aplurality of radiating elements of a periodic resonance structure. Thefirst fluid dielectric is controlled to selectively vary an electricallength of each of the transmission line stubs. This permits directing anangle of a redirected RF beam produced by an incident RF signalimpinging on the periodic resonance structure.

According to one aspect of the invention, the controlling step caninclude varying a volume of the first fluid dielectric coupled to thetransmission line stubs to control an electrical length of the pluralityof transmission line stubs. Selectively varying the volume can includethe steps of pumping a fluid dielectric into and out of a cavitystructure positioned adjacent to the transmission line stub. Inparticular, independently varying the volume of the first fluiddielectric can be used to control the beam angle of the redirected RFbeam.

When the volume of the first fluid dielectric is varied, it can displacea gas contained in said cavity structure or a second fluid dielectricalso contained within the cavity structure. If a second fluid dielectricis displaced, then the first and second fluid dielectrics can beselected to be immiscible.

According to another aspect of the invention, the step of selectivelycontrolling the fluid dielectric can be performed by increasing ordecreasing a volume of the fluid dielectric contained in the pluralityof cavity structures. Since the cavity structures are respectivelycoupled to the plurality of transmission line stubs, the variation inthe fluid volume can be used to vary an electrical length of theplurality of transmission line stubs.

According to another aspect, the invention can also include a steerablebeam antenna that operates in accordance with the above-describedmethod. More particularly, a periodic resonance structure can include aplurality of transmission line stubs respectively coupled to a pluralityof radiating elements. A plurality of cavity structures, each capable ofcontaining fluid dielectric, can be provided proximate to the stubs sothat the fluid dielectric is electrically and magnetically coupled tothe transmission line stubs. At least one fluid processor can beprovided for controlling the fluid dielectric. More particularly, thefluid processor can control the fluid dielectric to selectively vary anelectrical length of the transmission line stubs. In so doing, an angleof a redirected RF beam produced by an incident RF signal impinging onthe periodic resonance structure can be controlled to direct an antennabeam produced by the periodic resonance structure.

The fluid processor can comprises a controller and at least one pump forcontrolling a volume of the first fluid dielectric contained in thecavity structures so as to vary an electrical length of the transmissionline stubs. The first fluid dielectric displaces a gas or a second fluiddielectric contained in said cavity structure. However, if a secondfluid dielectric is used, the first and second fluid dielectrics can beimmiscible so that an immiscible fluid interface separates the first andsecond fluid dielectrics.

According to another aspect, the fluid processor can be configured tocontrol the fluid dielectric by selectively increasing and decreasing avolume of fluid dielectric contained in the plurality of cavitystructures respectively coupled to the transmission line stubs.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 is a top view of a single element of a periodic resonancestructure type antenna that can be controlled with a fluid dielectric.

FIG. 2 is a cross-sectional view of the element of FIG. 1.

FIG. 3 is a perspective view of a periodic resonance structureincorporating the element of FIGS. 1 and 3.

FIG. 4 is a flowchart that is useful for understanding a method forsteering an antenna beam using a periodic resonance structure.

DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS

FIGS. 1 and 2 illustrate a single element 100 which can be used to forma steered beam periodic resonance structure. FIG. 1 is a top view of theelement 100 and FIG. 2 is a cross-sectional view of the element 100taken along line 2-2 in FIG. 1. The element 100 in FIG. 1 is comprisedof a radiating element 102 closely spaced above an electricallyconducting ground plane 110. In the exemplary embodiment of FIGS. 1 and2, the radiating element 102 is a conventional patch antenna and canhave a resonant dimension of one half wavelength. According to apreferred embodiment, the radiating element 102 can be disposed on adielectric substrate 101. The dielectric substrate can be any suitablematerial but is preferably a glass/ceramic substrate for reasons thatshall subsequently discussed in more detail.

Radiating element 102 as illustrated in FIGS. 1 and 2 are well known inthe art. However, it should be understood that the particular type ofradiating element illustrated is not essential to the invention and avariety of other types of radiating elements can also be used. Forexample, other shapes including square, rectangular, circular, andelliptical designs can also be used.

Referring again to FIGS. 1 and 2, it can be seen that the element 100includes an integrally formed microstrip transmission line stub 104. Thetransmission line stub is also preferably formed on the dielectricsubstrate 101 and is preferably coupled to an impedance matched feedpoint associated with radiating element 102. The transmission line stubcan be terminated as an open circuit or a short circuit termination at106. In FIGS. 1 and 2, an open circuit termination is shown. It shouldbe noted that while a microstrip type transmission line is shown inFIGS. 1 and 2, the invention is not so limited. Any convenient type oftransmission line stub can be used for this purpose. For example, thetransmission line stub can also be fabricated in a buried microstrip orstripline configuration.

RF radiation incident on the element 100 will be coupled to theradiating element 102 and will be converted to corresponding RFelectrical currents which propagate along the microstrip transmissionline stub 104, toward termination 106. Provided that termination 106 isan open circuit or a short circuit, the RF currents propagating alongthe transmission line stub 104 toward termination 106 will be reflectedback toward the radiating element 102 and re-radiated from the element.Those skilled in the art will readily appreciate that the electricallength of the transmission line stub 104 will introduce a phase shift inthe re-radiated signal. The amount of the phase shift will be a functionof the transmission line stub length and the type of termination.

A cavity structure 108 can be disposed below the transmission line stub104. The cavity structure 108 preferably includes a port 112 so that afluid dielectric 114 may be circulated or moved into and out of thecavity structure 108. The cavity structure can extend partly orcompletely between the conductive ground plane 110 and the transmissionline stub 104.

Notably, the transmission line stub 104 has a physical length and anelectrical length. The electrical length k (where k is preferably somefraction of a wavelength λ) will be determined by the physical length kλof the transmission line stub 104 and the electrical characteristics ofthe dielectric material below the line. Since the dielectric materialbelow the line is fluid dielectric 114, the electrical length of theline will depend upon the electrical characteristics of the fluiddielectric at every point below the transmission line stub 104. Byselectively controlling the fluid dielectric 114, the electrical length(and the resulting phase shift) can be varied.

Two important characteristics of dielectric materials are permittivity(sometimes called the relative permittivity or ε_(r)) and permeability(sometimes referred to as relative permeability or μ_(r)). Thepermittivity and permeability determine the propagation velocity of asignal, which is approximately inversely proportional to {squareroot}{square root over (με)}. The propagation velocity directly affectsthe electrical length of a transmission line and therefore the amount ofphase shift introduced to signals that traverse the line.

Further, ignoring loss, the characteristic impedance of a transmissionline, such as stripline or microstrip, is equal to {square root}{squareroot over (L_(l)/C_(l))} where L_(l) is the inductance per unit lengthand C_(l) is the capacitance per unit length. The values of L_(l) andC_(l) are generally determined by the permittivity and the permeabilityof the dielectric material(s) used to separate the transmission linestructures as well as the physical geometry and spacing of the linestructures. If permittivity and permeability are maintained in aconstant ratio, then the characteristic impedance of the line willremain the same, while the electrical length of the line will bechanged.

According to one embodiment, the fluid dielectric 114 can be selectivelycontrolled by controlling the volume of the fluid dielectric that iscontained within cavity structure 108. As shown in FIG. 2, the volume ofthe fluid dielectric 114 contained in cavity structure 108 can beincreased or decreased by means of a pump 116 in fluid communicationwith the cavity structure 108 and a reservoir 118. The pump 116 can be aconventional pump or a micro electro-mechanical device which canoptionally be integrated into the dielectric substrate 101. Similarly,reservoir 118 can be external to the dielectric substrate 101 or can beformed integral therewith. The pump 116 is preferably operableindependently in response to a pump control signal 120 from a centralcontrol unit 122.

According to one embodiment, the portion 115 of cavity structure 108 andreservoir 118 not occupied by fluid dielectric 114 can be occupied by aninert gas. Vent tube 113 allows displacement of any of the inert gascontained within the cavity structure 108. If the relative permeabilityor permittivity of the fluid dielectric is selected to be different ascompared to the inert gas, then increasing or decreasing the amount offluid dielectric 114 contained within the cavity structure 108 will varythe electrical length of the transmission line stub 104. In turn, thiswill selectively vary a phase shift of RF energy communicated on stub104.

According to an alternative embodiment, the portion 115 of the cavitystructure and reservoir 118 not occupied by the fluid dielectric 114 canbe occupied by a second fluid dielectric with electrical propertiesdifferent as compared to fluid dielectric 114. In that case, the secondfluid dielectric can be selected to be immiscible with the first fluiddielectric so as to define an immiscible fluid interface 123. An exampleof immiscible fluids would include oil and water.

According to a preferred embodiment, the relative permittivity andpermeability of the fluid dielectric are preferably selected so that theintroduction of such fluid dielectric into the cavity 108 does not alterthe characteristic impedance of the transmission line stub. This can beaccomplished by always maintaining a constant ratio of relativepermittivity to relative permeability.

Referring now to FIG. 3, there is shown a periodic resonance structure300 which is formed as an array of elements 100, each including atransmission line stub 104 as described above. An electrical length ofeach transmission line stub 104 can be independently varied in themanner described above in response to commands from controller 122. Ahorn 304 can be provided on a suitable bracket 302 and can be configuredfor receiving RF, transmitting RF or both. FIG. 3 illustrates that anincident RF signal 306 which has some angle of arrival relative to thesurface of substrate 101, can be redirected at a second angle to form aredirected beam 308. The precise mechanism by which the beam isredirected will be determined by the relative phase shift introduced tothe incident signal by each element 100 of the array 300. Additionaldetail regarding such beam steering techniques are described in U.S.Pat. No. 4,684,952, the disclosure of which is expressly incorporatedherein by reference.

Composition of the Fluidic Dielectric

The fluidic dielectric as described herein can be comprised of any fluidcomposition having the required characteristics of permittivity andpermeability as may be necessary for achieving a selected range of phaseshift. Those skilled in the art will recognize that one or morecomponent parts can be mixed together to produce a desired permeabilityand permittivity required for a particular phase shift and transmissionline characteristic impedance.

The fluidic dielectric 114 also preferably has a relatively low losstangent to minimize the amount of RF energy lost in each element.However, devices with higher loss may be acceptable in some instances sothis may not be a critical factor. Many applications also require abroadband response. Accordingly, it may be desirable in many instancesto select fluidic dielectrics that have a relatively constant responseover a broad range of frequencies.

Aside from the foregoing constraints, there are relatively few limits onthe range of materials that can be used to form the fluidic dielectric.Accordingly, those skilled in the art will recognize that the examplesof suitable fluidic dielectrics as shall be disclosed herein are merelyby way of example and are not intended to limit in any way the scope ofthe invention. Also, while component materials can be mixed in order toproduce the fluidic dielectric as described herein, it should be notedthat the invention is not so limited. Instead, the composition of thefluidic dielectric could be formed in other ways. All such techniqueswill be understood to be included within the scope of the invention.

Those skilled in the art will recognize that a nominal value ofpermittivity (ε_(r)) for fluids is approximately 2.0. However, thefluidic dielectric used herein can include fluids with higher values ofpermittivity. For example, the fluidic dielectric material could beselected to have a permittivity value of between 2.0 and about 58,depending upon the amount of phase shift required.

Similarly, the fluidic dielectric can have a wide range of permeabilityvalues. High levels of magnetic permeability are commonly observed inmagnetic metals such as Fe and Co. For example, solid alloys of thesematerials can exhibit levels of μ_(r) in excess of one thousand. Bycomparison, the permeability of fluids is nominally about 1.0 and theygenerally do not exhibit high levels of permeability. However, highpermeability can be achieved in a fluid by introducing metalparticles/elements to the fluid. For example typical magnetic fluidscomprise suspensions of ferro-magnetic particles in a conventionalindustrial solvent such as water, toluene, mineral oil, silicone, and soon. Other types of magnetic particles include metallic salts,organo-metallic compounds, and other derivatives, although Fe and Coparticles are most common. The size of the magnetic particles found insuch systems is known to vary to some extent. However, particles sizesin the range of 1 nm to 20 μm are common. The composition of particlescan be selected as necessary to achieve the required permeability in thefinal fluidic dielectric. Magnetic fluid compositions are typicallybetween about 50% to 90% particles by weight. Increasing the number ofparticles will generally increase the permeability.

More particularly, a hydrocarbon dielectric oil such as Vacuum Pump OilMSDS-12602 could be used to realize a low permittivity, low permeabilityfluid, low electrical loss fluid. A low permittivity, high permeabilityfluid may be realized by mixing same hydrocarbon fluid with magneticparticles such as magnetite manufactured by FerroTec Corporation ofNashua, N.H., or iron-nickel metal powders manufactured by LordCorporation of Cary, N.C. for use in ferrofluids and magnetoresrictive(MR) fluids. Additional ingredients such as surfactants may be includedto promote uniform dispersion of the particle. Fluids containingelectrically conductive magnetic particles require a mix ratio lowenough to ensure that no electrical path can be created in the mixture.Solvents such as formamide inherently posses a relatively highpermittivty.

Similar techniques could be used to produce fluidic dielectrics withhigher permittivity. For example, fluid permittivty could be increasedby adding high permittivity powders such as barium titanate manufacturedby Ferro Corporation of Cleveland, Ohio. For broadband applications, thefluids would not have significant resonances over the frequency band ofinterest.

RF Unit Structure, Materials and Fabrication

According to one aspect of the invention, the dielectric substrate 101can be formed from a ceramic material. For example, the dielectricstructure can be formed from a low temperature co-fired ceramic (LTCC).Processing and fabrication of RF circuits on LTCC is well known to thoseskilled in the art. LTCC is particularly well suited for the presentapplication because of its compatibility and resistance to attack from awide range of fluids. The material also has superior properties ofwetability and absorption as compared to other types of solid dielectricmaterial. These factors, plus LTCC's proven suitability formanufacturing miniaturized RF circuits, make it a natural choice for usein the present invention.

Beam Control Process

Referring now to FIG. 4, a process shall be described for controllingthe angle of a redirected RF beam using the periodic resonance structure300. In step 402 and 404, controller 122 can wait for an antenna controlsignal 137 indicating a requested angle for a redirected beam. Once thisinformation has been received, the controller 122 can determine in step406 a required phase shift for each transmission line stub 104 and arequired amount of fluid dielectric 114 that is needed for each cavitystructure 108 in order to produce the required phase shift. In step 408,the controller 122 can selectively control pumps 116 associated witheach element 100 to produce the required phase shift.

As an alternative to calculating the required configuration of the fluiddielectric, the controller 122 could also make use of a look-up-table(LUT). The LUT can contain cross-reference information for determiningcontrol data for each element 100 necessary to achieve variousredirected beam angles. For example, a calibration process could be usedto identify the specific digital control signal values communicated fromcontroller 122 to each of the pumps 116 that are necessary to achieve aspecific angle for the redirected beam. These digital control signalvalues could then be stored in the LUT. Thereafter, when control signal137 is updated, the controller 122 can immediately obtain thecorresponding digital control signal for producing the required beam.

As an alternative, or in addition to the foregoing methods, thecontroller 122 could make use of an empirical approach that applies areference signal to each radiating element and then measures the phaseshift that occurs at each element 100. Specifically, the controller 122can check to see whether the updated phase shift for each element hasbeen achieved. A feedback loop could then be employed to control thepumps 116 to produce the desired redirected beam angle.

While the preferred embodiments of the invention have been illustratedand described, it will be clear that the invention is not so limited.Numerous modifications, changes, variations, substitutions andequivalents will occur to those skilled in the art without departingfrom the spirit and scope of the present invention as described in theclaims.

1. A method for steering an antenna beam using a periodic resonancestructure, comprising the steps of: electrically and magneticallycoupling a first fluid dielectric to a plurality of transmission linestubs that are respectively coupled to a plurality of radiating elementsof a periodic resonance structure; and controlling said first fluiddielectric to selectively vary an electrical length of said plurality oftransmission line stubs, whereby an angle can be controlled for aredirected RF beam produced by an incident RF signal impinging on saidperiodic resonance.
 2. The method according to claim 1 wherein saidcontrolling step further comprises the step of varying a volume of saidfirst fluid dielectric coupled to said transmission line stubs tocontrol an electrical length of said plurality of transmission linestubs.
 3. The method according to claim 2 wherein said step ofselectively varying said volume includes pumping a fluid dielectric intoand out of a cavity structure positioned adjacent to said transmissionline stub.
 4. The method according to claim 2 further comprising thestep of independently varying said volume of said first fluid dielectriccoupled to each of said plurality of transmission line stubs to controlsaid angle of said redirected RF beam.
 5. The method according to claim2 wherein said step of varying said volume further comprises displacingwith said first fluid dielectric a gas contained in said cavitystructure.
 6. The method according to claim 2 wherein said step ofvarying said volume further comprises displacing with said first fluiddielectric a second fluid dielectric also contained within said cavitystructure.
 7. The method according to claim 6 further comprising thestep of selecting said first and second fluid dielectrics to beimmiscible.
 8. The method according to claim 1 wherein said step ofselectively controlling said fluid dielectric further comprisescontrolling a presence or removal of a volume of said first fluiddielectric from a plurality of cavity structures respectively coupled tosaid plurality of transmission line stubs for controlling an electricallength of said plurality of transmission line stubs.
 9. A steerable beamantenna comprising: a periodic resonance structure comprising aplurality of transmission line stubs respectively coupled to a pluralityof radiating elements; a plurality of cavity structures each containingat least a first fluid dielectric, said first fluid dielectricelectrically and magnetically coupled to said transmission line stubs;and at least one fluid processor controlling said fluid dielectric forselectively varying an electrical length of said transmission linestubs, whereby an angle of a redirected RF beam produced by an incidentRF signal impinging on said periodic resonance structure can becontrolled.
 10. The steerable beam antenna according to claim 9 whereinsaid fluid processor comprises a controller and at least one pump forcontrolling a volume of said first fluid dielectric in said cavitystructures to vary an electrical length of said plurality oftransmission line stubs.
 11. The steerable beam antenna according toclaim 10 wherein said first fluid dielectric displaces a gas in saidcavity structures.
 12. The steerable beam antenna according to claim 10wherein said first fluid dielectric displaces a second fluid dielectricin said cavity structure.
 13. The steerable beam antenna according toclaim 12 wherein said first and second fluid dielectrics are immiscible.14. The steerable beam antenna according to claim 13 wherein animmiscible fluid interface separates the first and second fluiddielectrics.
 15. The steerable beam antenna according to claim 9 whereinsaid fluid processor controls said first fluid dielectric byindependently increasing and decreasing a volume of said first fluiddielectric contained in said plurality of cavity structures respectivelycoupled to said plurality of transmission line stubs.
 16. The steerablebeam antenna according to claim 9 wherein said periodic resonancestructure is an array of patch antennas.